Image stabilizing apparatus and optical apparatus

ABSTRACT

An image stabilizing apparatus is disclosed which is capable of sufficiently correcting shift shakes even with a small and lightweight accelerometer. The apparatus includes an angular velocity detector which detects angular velocity generated by a shake, an angular velocity computing unit which processes an angular velocity signal, the unit processing the angular velocity signal with a first frequency characteristic, an acceleration detector which detects acceleration generated by the shake, an acceleration computing unit which processes an acceleration signal, the unit processing the acceleration signal with a second frequency characteristic having a signal processing band narrower than the first frequency characteristic, an adder which adds an output signal from the angular velocity computing unit to an output signal from the acceleration computing unit, and an image stabilizing mechanism which performs an image stabilizing operation based on an output signal from the adder.

BACKGROUND OF THE INVENTION

The present invention relates to an image stabilizing apparatus thatcorrects an image shake due to, for example, a hand shake to preventdegradation of a picked-up image, and an optical apparatus having theimage stabilizing apparatus.

In current cameras, all important tasks for image pickup such asexposure decisions, focusing and the like are automated, so that evenamateurs in camera operation are much less likely to fail in imagepickup.

Recently, cameras provided with a system for preventing an image shakedue to a hand shake have also been put on the market, virtuallyeliminating any factors that cause a photographer to fail in imagepickup.

An apparatus for correcting image shakes, also referred to as imagestabilizing apparatus, will now be briefly described.

A hand shake on a camera in image pickup is typically a shake from 1 Hzto 10 Hz in terms of a frequency.

In order to ensure that the camera can pick up an image without an imageshake even if such a hand shake occurs when the shutter is released, theshake of the camera due to the hand shake must be detected and an imagecorrection lens must be moved depending on the detected value.

Therefore, in order to pick up an image without the image shake even ifa camera shake occurs, firstly the shake of the camera must beaccurately detected, and secondly, the variation of the optical axis dueto the hand shake must be corrected.

The detection of the shake (or camera shake) can be accomplished with ashake detector mounted on the camera. Fundamentally, the detectordetects the acceleration, angular acceleration, angular velocity,angular displacement and the like, and appropriately computes the outputfor camera shake correction.

Based on the detection information, the image stabilizing apparatus thatdecenters the image pickup optical axis is driven to correct the imageshake.

FIG. 10A shows a plan view of a conventional single-lens reflex camera,and FIG. 10B shows a side view of the same.

An image stabilizing system mounted on an interchangeable lens 90 thatconstitutes a part of the single-lens reflex camera system corrects animage due to camera shakes in the pitch and yaw directions indicated byarrows 92 p and 92 y, respectively, relative to an optical axis 91.

Incidentally, reference character 93 a denotes a release member (orrelease button), 93 b denotes a mode dial (including a main switch), 93c denotes a retractable flash, and 93 d denotes a camera CPU provided ina camera body 93.

In FIGS. 10A and 10B, reference character 94 denotes an image pickupelement, and 95 denotes an image stabilizing mechanism (or imagestabilizer) that drives a correction lens 95 a in the directions ofarrows 95 p and 95 y in FIG. 10 to correct the shakes in the directionsof arrows 92 p and 92 y. Reference characters 96 p and 96 y denoteangular velocity meters that detect the shakes in the directions ofarrows 92 p and 92 y, respectively. Arrows 96 pa and 96 ya indicate therespective sensitivity directions.

The output signals from the angular velocity meters 96 p and 96 y areinput to a lens CPU 97 and converted thereby to a shake correctiontarget value for the image stabilizing mechanism.

In synchronism with a half-press operation (which is hereinafterreferred to as S1 and an operation that instructs the camera to performphotometering and focusing for the preparation of image pickup) of therelease member 93 a provided on the camera body 93, the shake correctiontarget value is input to a coil in the image stabilizing mechanismthrough an image stabilizing driver 98 to start the shake correction.

The image stabilizing system illustrated in FIG. 10 uses the angularvelocity meters 96 p and 96 y to detect hand shakes.

The camera body 93 is subjected not only to rotational shakes in thedirections of arrows 92 p and 92 y but also to translational shakesindicated by arrows 11 yb and 11 pb. However, under a typical imagepickup condition, the rotational shakes in the directions of arrows 92 pand 92 y are dominant, and the translational shakes indicated by arrows11 yb and 11 pb cause less degradation of images.

Therefore, it is sufficient to provide only angular velocity meters 96 pand 96 y to detect hand shakes.

However, the degradation of images due to the translational shakes(hereinafter referred to as shift shakes) indicated by arrows 11 yb and11 pb can not be ignored in close-up image pickup (or under an imagepickup condition with large image pickup magnification).

For example, under a condition, such as macro image pickup, in which animage is picked up near a subject in the range on the order of 20 cm, orwhen the image pickup optical system has a very large focal length (forexample, 400 mm) although the subject is located in the range on theorder of 1 m, it is necessary to actively detect the shift shakes todrive the image stabilizing apparatus.

In Japanese Patent Laid-Open No. H07-225405, there has been disclosed atechnique in which an accelerometer for detecting the acceleration isprovided, and the shift shake is detected by the accelerometer to drivean image stabilizing apparatus along with an output from an angularvelocity meter provided otherwise.

In the technique disclosed in the Japanese Patent Laid-Open No.H07-225405, the lens CPU converts the angular velocity meter output intoan angle through a single integration, and converts the accelerometeroutput into a displacement through a double integration.

The integration operations suffer from the accumulation of slight errorsin input signals, and the errors may significantly grow in the case ofthe double integration.

Therefore, an accelerometer that needs a double integration is requiredto be highly accurate.

However, there is a problem that such a highly accurate accelerometer istypically large and heavyweight and is not suitable for use in aconsumer product.

BRIEF SUMMARY OF THE INVENTION

The present invention provides an image stabilizing apparatus capable ofsufficiently correcting shift shakes even with a small and lightweightaccelerometer, and an optical apparatus using the same.

According to one aspect, the present invention provides an imagestabilizing apparatus which includes an angular velocity detector whichdetects angular velocity generated by a shake, an angular velocitycomputing unit which processes an angular velocity signal obtained bythe angular velocity detector, the angular velocity computing unitprocessing the angular velocity signal with a first frequencycharacteristic, an acceleration detector which detects accelerationgenerated by the shake, an acceleration computing unit which processesan acceleration signal obtained by the acceleration detector, theacceleration computing unit processing the acceleration signal with asecond frequency characteristic having a signal processing band narrowerthan the first frequency characteristic, an adder which adds an outputsignal from the angular velocity computing unit to an output signal fromthe acceleration computing unit, and an image stabilizing mechanismwhich performs an image stabilizing operation based on an output signalfrom the adder.

According to another aspect, the present invention provides an opticalapparatus including the abovedescribed image stabilizing apparatus.

Other objects and features of the invention will be apparent from thepreferred embodiments described below with reference to the drawings.

BRIEF DESCRIPTION OF THE DRAWINGS

FIGS. 1A and 1B show a top view and a side view illustrating a digitalsingle-lens reflex camera that is Embodiment 1 of the present invention,respectively;

FIG. 2 shows a block diagram illustrating a circuit configuration ofEmbodiment 1;

FIGS. 3A to 3C illustrate gravitational errors added to an accelerometerin Embodiment 1;

FIG. 4 illustrates a gravitational error depending on a shake angle inEmbodiment 1;

FIG. 5 shows a flow chart illustrating the operation of the camera inEmbodiment 1;

FIGS. 6A to 6D illustrate the frequency characteristics of anacceleration computing unit and an angular velocity computing unit inEmbodiment 1;

FIG. 7 illustrates the frequency characteristics of shift shakes;

FIGS. 8A and 8B illustrate the frequency characteristics of anacceleration computing unit in Embodiment 2 of the present invention;

FIG. 9 illustrates an exemplary circuit configuration of an amplifier inEmbodiment 3 of the present invention; and

FIGS. 10A and 10B show a top view and a side view of a conventionaldigital single-lens reflex camera, respectively.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

The preferred embodiments of the present invention will now be describedwith reference to the accompanying drawings.

Embodiment 1

FIGS. 1A and 1B show a top view and a side view of a digital single-lensreflex camera system that is Embodiment 1 of the present invention,composed of an interchangeable lens (or optical apparatus, hereinaftersimply referred to as a lens) 90 provided with an image stabilizingapparatus, and a camera body 93 on which the lens 90 is removablymounted.

In this embodiment, components identical to those of the conventionalcamera system shown in FIGS. 10A and 10B are designated with the samereference characters. The embodiment is different from the conventionalcamera system in that the lens 90 is provided with accelerometers 11 pand 11 y in addition to angular velocity meters 96 p and 96 y.

The detecting axes of the accelerometers 11 p and 11 y are shown byarrows 11 pa and 11 ya, respectively. Reference character 99 denotes afocus lens, and multiple lens units including this focus lens constitutean image pickup optical system.

FIG. 2 shows a block diagram illustrating a configuration of a circuitthat processes signals of shift shakes detected by the accelerometers 11p and 11 y and rotational shakes detected by the angular velocity meters96 p and 96 y. The signals are mostly processed in a lens CPU 97.

FIG. 2 shows only a signal processing flow for correcting an image shakedue to a camera shake in the pitch direction (i.e. the rotational shake92 p and the shift shake 11 pb in FIG. 1B). In practice, however, animage shake due to a camera shake in the yaw direction (i.e. therotational shake 92 y and the shift shake 11 yb in FIG. 1A) is alsocorrected in a similar signal processing flow.

In FIG. 2, a shake angular velocity signal from the angular velocitymeter 96 p is input to an amplifier 12 p.

The amplifier 12 p amplifies output from the angular velocity meter 96 pand is provided with a DC removing circuit for removing a direct current(DC) component and a high-frequency attenuation circuit for removing ahigh-frequency noise component, the components being superimposed on theoutput of the angular velocity meter 96 p.

The output from the amplifier 12 p is A/D converted and taken into thelens CPU 97.

The taken signal will be digitally processed in the lens CPU 97. Here,the process is shown divided into respective blocks for illustrativepurpose.

An angular velocity integrator 13 p performs single integration on ashake angular velocity signal input from the amplifier 12 p to convertit into a shake angle.

The angular velocity integrator 13 p typically integrates high frequencycomponents of approximately 0.1 Hz or higher of a shake angular velocitysignal to convert it to a shake angle signal.

However, at the start of the angular velocity integration, theintegration band is narrowed (for example, signals of 2 Hz or lower areattenuated) to accelerate activation of the signal processing (which isreferred to as time-constant switching).

The resulting shake angle signal is input to an adder 14 p, and added toa shake displacement signal described below to generate a total shakesignal.

The adder 14 p adds the shake angle signal to the shake displacementsignal described below based on signals from a release member 93 a and afocus detector 27, described below.

The shake angle signal is input to the adder 14 p in response to thehalf-press operation S1 (an operation for photometering and focusing) ofthe release member 93 a. The adder 14 p adds the shake displacementsignal to the shake angle signal based on a signal input (indicatingcompletion of focusing) from the focus detector 27 to generate the totalshake signal.

The total shake signal is input to a frequency characteristic changer 15p to alter the frequency characteristics.

The frequency characteristic changer 15 p mainly attenuates lowfrequency components of the total shake signal. The frequencycharacteristic changer 15 p determines a frequency (for example, 0.1 Hzor 5 Hz) below which any frequencies are subjected to the attenuationand attenuates the signal components of the frequencies.

This is for preventing shake correction, that is, image stabilization,by increasing the level of attenuation of the total shake signal (forexample, by attenuating signals of 5 Hz or lower) when a large shakesuch as a camera framing change occurs.

Without the frequency characteristic changer 15 p, good camera framingcannot be achieved because even camera framing components are subjectedto the shake correction.

The output from the frequency characteristic changer 15 p is input to asensitivity changer 16 p.

The sensitivity changer 16 p receives signals from a focal lengthdetector 18 and an image pickup distance detector 19, which are input tothe lens CPU 97, to alter the amplification factor (or gain) for thesignal from the frequency characteristic changer 15 p.

Here, the shake correction sensitivity of the correction lens 95 a,which is included in the image pickup optical system as a zoom lens asshown in the embodiment, varies depending on a zooming state or afocusing state.

For example, when the correction lens 95 a driven by 1 mm on thewide-angle side causes an image shift of 1 mm on an image plane, thecorrection lens 95 a driven by 1 mm on the telephoto side causes animage shift of 3 mm on the image plane.

Similarly, the relationship between the movement amount of thecorrection lens 95 a and the amount of image shift varies whether asubject is closely located or a subject is located in infinity.

Therefore, in order to correct the sensitivity, the amplification factorfor the signal from the frequency characteristic changer 15 p is altereddepending on the zooming state or the focusing state (for example, theamplification factor on the telephoto side is reduced to one-third ofthat on the wide-angle side)

The focal length detector 18 is provided in the lens 90 and is anencoder and the like that detects the position of a magnificationvarying lens (not shown) which is moved when zooming. The focal lengthis detected using output from the encoder or the like.

The image pickup distance detector 19 is also provided in the lens 90and is an encoder and the like that detects the position of a focus lens99 which is moved when focusing. The image pickup distance is detectedusing output from the encoder or the like.

With an operation (half-press operation S1) of the release member 93 afor preparation of image pickup, a shake correction target signal fromthe sensitivity changer 16 p is converted to a PWM signal and input tothe image stabilizing driver 98 p.

The image stabilizing driver 98 p operates the image stabilizingmechanism 95 (that is, the correction lens 95 a) in response to theinput PWM signal so that the mechanism shifts relative to the opticalaxis 91 to effect the shake correction.

At this time, only a shake angle signal is input to the adder 14 p, andtherefore, only the rotational shake is corrected.

In addition, in response to a half-press signal generated by thehalf-press operation S1 of the release member 93 p, the focus detector27 in the camera CPU 93 d activates a focusing sensor 32 in the camerabody 93 to detect the focusing state with respect to a subject.

Depending on the detected result of the focusing sensor 32, the focusdetector 27 sends the amount of out-of-focus to a lens drive computingunit 33 in the lens CPU 97.

The lens drive computing unit 33 drives a focus actuator 34 based on thesignal to move the focus lens 99.

Here, since the rotational shake is being corrected during the focusingoperation as described above, highly accurate focusing operation can beachieved.

After the drive of the focus lens 99, the focusing sensor 32 againdetects the focusing state, and the camera CPU 93 d provides an in-focusindication if a sufficient focusing state (or an in-focus state) isobtained. On the other hand, the camera CPU 93 d moves the focus lens 99again if the sufficient focusing state is not obtained.

In the sufficient focusing state, the focus detector 27 causes the adder14 p to add the shake displacement signal to the shake angle signal.

Although the movement amount of the focus lens 99 is continuously inputto the sensitivity changer 16 p, the sensitivity changer 16 p uses asthe sensitivity value the movement amount of the focus lens 99 at thetime of the focus detector 27 detecting the in-focus state.

The image magnification is computed from the relationship between themovement amount of the focus lens 99 and the position of themagnification varying lens, and the computation of the imagemagnification is started using the in-focus detection by the focusdetector 27 as a trigger, as described below.

That is, when the zooming state is fixed (it is assumed that the zoomingstate is fixed before the half-press operation S1 of the release member93 a by the photographer) and the focusing state is in focus on thesubject and thereby the movement amount of the focus lens 99 isdetermined, the sensitivity for the shake correction is determined andthen the shake correction target value is calculated.

The image magnification is also determined when the focusing state is infocus on the subject.

The shake correction target signal determined as described above, givenby adding the shake displacement signal to the shake angle signal, isconverted to a PWM signal, and then the PWM signal is input to the imagestabilizing driver 98 p.

The image stabilizing driver 98 p activates the image stabilizingmechanism 95 (that is, the correction lens 95 a) in response to theinput of the PWM signal to perform the shake correction.

In other words, upon the completion of focusing, the shift shake is alsocorrected.

The signal processing for an accelerometer 11 p will now be described.

A shake acceleration signal output from the accelerometer 11 p is inputto an amplifier 20 p.

The amplifier 20 p amplifies output from the accelerometer 11 p and isprovided with a DC removing circuit for removing a DC component and ahigh-frequency attenuation circuit for removing a high-frequency noisecomponent, the components being superimposed on the output of theaccelerometer 11 p.

The output from the amplifier 20 p is A/D converted and taken into thelens CPU 97.

The taken shake acceleration signal will also be digitally processed inthe lens CPU 97. Again, the process is shown divided into respectiveblocks for illustrative purpose.

First, the shake acceleration signal is input to an acceleration gravitycorrector 21 p to perform correction of a gravitational component.

Here, description will be made what the correction of gravitationalcomponent means.

At the image pickup position of the camera shown in FIG. 1B, thesensitivity direction 11 pa of the accelerometer 11 p is the same as thedirection of the gravity 28 because the camera is horizontal (see FIG.3A).

At this time, the accelerometer 11 p continuously outputs a signalcorresponding to the gravitational component, and a shift shakecomponent is detected from the signal superimposed on the gravitationalcomponent.

Since an output signal of the gravitational component is a DC component,it can be removed by the DC removing circuit and the like in theamplifier 20 p.

However, the position of the accelerometer 11 p varies as indicated by adashed line in FIG. 3A due to a change in a rotating angle of a handshake generated when the camera is gripped, so that the direction of thegravity will vary as viewed from the accelerometer 11 p.

Therefore, the output from the accelerometer 11 p varies due to a changein the shake angle.

FIG. 3C shows a variation of the output from the accelerometer 11 p withrespect to a posture (or shake rotating angle θ) of the accelerometer 11p; the horizontal axis shows a posture variation of the accelerometer 11p and the vertical axis shows the output from the accelerometer 11 p.

A graph 30 p shows the output from the accelerometer 11 p. As theposture angle of the accelerometer 11 p increases or decreases from zero(a state when 1 G is applied as shown in FIG. 3A) by ±θ, the output fromthe accelerometer 11 p changes (or decreases).

FIG. 4 shows the output from the accelerometer 11 p with a gravitationalvariation where the horizontal axis shows elapsed time after the camerais gripped and the vertical axis shows the shake rotating angle and theoutput from the accelerometer 11 p.

Assuming there is no shift shake, the accelerometer 11 p still outputsan error signal 30 p due to a variation in the gravitational componentgenerated depending on a shake rotating angle 29 p.

In close-up image pickup, the camera is often tilted down to pick up animage. FIG. 3B shows such a case, and the direction of the gravity 28 isperpendicular to the sensitivity direction 11 pa of the accelerometer 11p.

In this case, the error signal is as indicated by dashed line graph 31 pshown in FIGS. 3C and 4.

Here, there is a difference in the level of the error signals 30 p and31 p between the position of the accelerometer 11 p in FIG. 3A and theposition of the accelerometer 11 p in FIG. 3B because the gravityaffects the error signal in a cosine manner with respect to a change inthe shake angle at the position in FIG. 3A. At the position in FIG. 3B,the gravity affects the error signal in a sine manner, and the variationwill be larger in the sine manner when the angle of posture change issmall.

Therefore, in order to correct (remove) the gravitational effect, it isnecessary to detect the shake angle and the posture (or the sensitivityaxis angle with respect to the gravity as shown in FIGS. 3A and 3B) ofthe accelerometer 11 p.

Returning to FIG. 2, a half-press signal from the release member 93 a isinput to the lens CPU 97 through the camera CPU 93 d.

The half-press operation S1 is performed after the camera is pointed ata subject for the preparation of image pickup and an image compositionis fixed, and the half-press signal causes photometering and focusingwith respect to the subject to start.

In FIG. 2, the above operations are omitted because they are notdirectly relevant to the feature of this embodiment, and the half-presssignal from the release member 93 a is input to an initial posture anddirection detector 23 p through the camera CPU 93 d.

The initial posture and direction detector 23 p also receives an inputof an amplified acceleration signal from the amplifier 20 p, anddetermines the posture of accelerometer 11 p according to the magnitudeof the amplified acceleration signal when the half-press signal from therelease member 93 a is input.

Since the half-press operation S1 on the release member 93 a is a buttonmanipulation performed by a photographer after the image composition isfixed, the posture is not widely changed thereafter.

Therefore, it is effective to determine the posture of the accelerometer11 p based on the amplified acceleration signal.

The posture may of course be detected after the half-press operation S1and then the camera focuses on a subject. In this case, however, theintegration of the output from the accelerometer 11 p (described below)cannot be performed using the time interval between the half-pressoperation S1 and focusing.

Therefore, it is desirable to detect the posture of the accelerometer 11p during the half-press operation S1 in order also to save time.

Specifically, it is determined that the accelerometer 11 p has theposture shown in FIG. 3A when the magnitude of the acceleration is 1 Gupon input of the half-press signal, that it has the posture shown inFIG. 3B when it is 0 G, and that it has a posture corresponding to anacceleration between 1 G and 0 G.

The shake angle signal from the angular velocity integrator 13 p isinput not only to the abovedescribed adder 14 p but also to agravitational effect calculator 24 p.

The gravitational effect calculator 24 p calculates a variation in thegravity acting on the accelerometer 11 p based on a change in the inputshake angle signal. As described above, the calculation varies dependingon the posture of the accelerometer 11 p with respect to the gravity,that is, depending on whether the sine manner or the cosine manner isused in the calculation.

Therefore, a signal from the initial posture and direction detector 23 pis also input to the gravitational effect calculator 24 p to change acoefficient in the calculation between the posture shown in FIG. 3A andthe posture shown in FIG. 3B.

Specifically, when the posture φ is zero degree while 1 G is applied asshown in FIG. 3A and a change in the posture (or shake rotating angle)is θ, the change in output from the accelerometer 11 p is determined as:

G{cos φ−cos(φ+θ)}.

Therefore, an initial posture φ determined by the initial posture anddirection detector 23 p and a current shake angle are used to determinea posture change θ, which is used to calculate a gravitational effect.

The amplified acceleration signal from the amplifier 20 p is input tothe acceleration gravity corrector 21 p, where the amplifiedacceleration signal is used to calculate the difference from the signalfrom the accelerometer 11 p which is changed in association with agravitational variation obtained by the gravitational effect calculator24 p to remove an output error in the accelerometer 11 p due to thegravity.

A shake acceleration signal after removal of the error component isinput to an acceleration integrator 22 p.

The acceleration integrator 22 p performs a double integration on theshake acceleration signal in which the gravitational effect wascorrected by the acceleration gravity corrector 21 p to convert theshake acceleration signal to a shake displacement.

Similarly to the angular velocity integrator 13 p, the accelerationintegrator 22 p typically performs a double integration on a highfrequency component of 0.4 Hz or higher of the shake acceleration signalto convert the high frequency component to the shake displacement.

At the start of the acceleration signal integration, the accelerationintegrator 22 p narrows the integration band (for example, only acomponent of 1 Hz or higher is integrated) to accelerate activation ofthe signal processing (i.e. time-constant switching).

The shake displacement signal from the acceleration integrator 22 p isinput to an image magnification corrector 25 p.

An image pickup magnification computing unit 26 p calculates an imagepickup magnification based on focal length information from the focallength detector 18 and image pickup distance information from the imagepickup distance detector 19.

As described above, the focal length detector 18 is provided in the lens90 and is an encoder and the like that detects the position of themagnification varying lens which is moved when zooming. The focal lengthis detected using output from the encoder or the like.

The image pickup distance detector 19 is also provided in the lens 90.

The image pickup distance detector 19 is an encoder and the like thatdetects the position of the focus lens 99 which is moved when focusing.The image pickup distance is detected using output from the encoder orthe like.

The focus lens 99 is driven based on information on the amount ofout-of-focus from the focus detector 27 as described above, and afterthe completion of the drive and when the focus detector 27 confirms anin-focus state, the image pickup magnification computing unit 26 pcomputes an image pickup magnification based on the outputs from thefocal length detector 18 and the image pickup distance detector 19.

The shift shakes 11 pb and 11 yb will have a large effect on a picked-upimage when a subject is closely located and the image pickup focallength is large (i.e. in the case of a large image pickupmagnification), and have a much less effect on the picked-up image whenthe subject is distantly located (i.e. in the case of a small imagepickup magnification).

Therefore, it is necessary to amplify the shake displacements (or theshift shakes), which have been detected by the accelerometers 11 p and11 y and then computed, depending on the image pickup magnification toobtain shake correction target values.

The image magnification corrector 25 p amplifies the shake displacementfrom the acceleration integrator 22 p based on a computed value(computed assuming that the image pickup magnification is large when thefocal length is large and the subject is closely located) from the imagepickup magnification computing unit 26 p.

The adder 14 p adds the signal from the angular velocity integrator 13 pto the signal from the image magnification corrector 25 p (the signalbased on the acceleration integrator 22 p). However, substantially onlythe output from the angular velocity integrator 13 p will remain whenthe subject is distantly located and the image pickup focal length issmall, as described above.

The operation following the adder 14 p is as described above: the outputfrom the adder 14 p is converted to a shake correction target valuethrough the frequency characteristic changer 15 p that facilitates acamera framing change and the sensitivity changer 16 p that adjusts theeffectiveness of the shake correction depending on the sensitivity ofthe correction lens 95 a, and is used to drive the image stabilizingmechanism 95.

FIG. 5 shows a flow chart illustrating the operation of theconfiguration described above. The flow starts when the main power ofthe camera body 93 is turned on and power supply to the lens 90 isstarted.

Various control steps provided for the camera (for example, batterychecking, photometering, focus detection, drive of the focus lens forauto-focusing, charging for flashing, and manipulations and operationsfor exposure) are omitted for clear understanding of major operations ofEmbodiment 1.

In this flow, description will be made of an example case where therotational shake 92 p and the shift shake 11 pb of the camera aredetected by the angular velocity meter 96 p and the accelerometer 11 p,respectively. However, a similar flow may be applied to the case wherethe rotational shake 92 y and the shift shake 11 yb of the camera aredetected by the angular velocity meter 96 y and the accelerometer 11 y,respectively.

At step S1001, the half-press operation S1 of the release member 93 a iswaited for, and upon the half-press operation S1, the flow proceeds tostep S1002.

At step S1002, the initial posture and direction detector 23 p detectsthe posture of the camera according to a signal from the accelerometer11 p.

This detects a gravity acceleration acting on the accelerometers 11 pand 11 y, and as shown in FIGS. 1A and 1B for example, the accelerometer11 p outputs a signal corresponding to 1 G and the accelerometer 11 youtputs a signal corresponding to 0 G when the camera is horizontallygripped.

At this time, if the camera is turned to be in a vertical posture (i.e.the right and left sides of the camera towards up and down), theaccelerometer 11 p outputs a signal corresponding to 0 G and theaccelerometer 11 y outputs a signal corresponding to 1 G.

When the camera is tilted down or up, both the accelerometers 11 p and11 y output signals corresponding to 0 G.

The posture is detected at the time of the half-press operation S1 ofthe release member 93 a because a photographer tends to first grip thecamera, fix the framing, and then perform the half-press operation S1after the camera is stabilized, so that the posture may not be oftenchanged thereafter.

If it is determined that the posture is as shown in FIG. 1A based on thesignals from the accelerometers 11 p and 11 y, gravity correction isapplied to the accelerometer 11 p. However, a gravitational effectcalculator 24 y determines that the gravity correction is not applied tothe accelerometer 11 y, and nulls the correction amount for anacceleration gravity corrector 21 y. This is because there isessentially no variation in the gravity acceleration due to rotationalshakes.

Therefore, the acceleration gravity corrector 21 y (not shown and havingthe similar configuration to the acceleration gravity corrector 21 p inorder to correct a gravitational effect on the accelerometer 11 y) doesnot perform a gravitational component correction (or the gravitycorrection) on an amplified signal from the accelerometer 11 y.

In contrast, when the camera is in another vertical posture (theaccelerometer 11 p→0 G; the accelerometer 11 y→1 G), the gravitycorrection is applied to the accelerometer 11 y based on the signal fromthe angular velocity meter 96 y, while the gravity correction is notapplied to the accelerometer 11 p based on the signal from the angularvelocity meter 96 p.

The gravitational effect calculator 24 p nulls the correction amount forthe acceleration gravity corrector 21 p.

When the camera is tilted down or up (the accelerometer 11 p→±1 G; theaccelerometer 11 y→±1 G), the gravity correction is applied to theaccelerometer 11 p based on the signal from the angular velocity meter96 p, and the gravity correction is applied to the accelerometer 11 ybased on the signal from the angular velocity meter 96 y.

In this way, it is determined whether or not the gravity correction isperformed depending on the posture.

In addition to the gravity acceleration, an acceleration due to theshift shake is superimposed on the signals from accelerometers 11 p and11 y.

Therefore, each signal from each of the accelerometers 11 p and 11 y isaveraged for a predetermined time (for example, 1 second) to obtain onlya gravitational component.

When the posture detection is completed in this way, the flow proceedsto step S1003.

At step S1003, sensitivity correction depending on the state of thefocus lens 99 and frequency correction depending on the state of theshake (such as panning) are applied to the shake angle signal.

At step S1004, the rotational shake correction is performed based on theshake angle signal.

At step S1005, the gravitational effect calculator 24 p calculates thegravity acceleration acting on the accelerometer 11 p based on theposture of the camera detected by the initial posture and directiondetector 23 p and the shake angle information from the angular velocityintegrator 13 p, and the acceleration gravity corrector 21 p correctsthe error output.

At step S1006, focusing is started.

At step S1007, completion of the lens movement for focusing is waitedfor. The wait time continues until the focus detector 27 detects thein-focus state, the lens drive computing unit 33 computes the lensmovement amount, the focus lens actuator 34 drives the focus lens 99,and then the focusing sensor 32 confirms that the in-focus state on asubject is achieved.

At step S1008, the position of the focus lens 99 is read by the focusencoder that is the image pickup distance detector 19 upon completion ofthe drive of the focus lens 99 at step S1007 to detect the image pickupdistance (or object distance).

At step S1009, focal length information of the lens 90 is detected bythe zoom encoder that is the focal length detector 18, and the imagepickup magnification computing unit 26 p computes the image pickupmagnification in relation to the image pickup distance determined atstep S1008. The image magnification corrector 25 p then alters the gainfor the shake displacement obtained by the acceleration integrator 22 p,based on the result from the image pickup magnification computing unit26 p.

The resulting shake displacement is added to the shake angle signal fromthe angular velocity integrator 13 p by the adder 14 p. The frequencycharacteristic changer 15 p to which the addition output is inputchanges the shake correction frequency band depending on the imagepickup condition. The sensitivity changer 16 p alters the gain for theoutput in which the shake correction frequency band was changed, basedon the abovedescribed shake correction sensitivity determined based onthe detection results from the focal length detector 18 and the imagepickup distance detector 19, and thereby the shake correction targetvalue is calculated.

At step S1010, the image stabilizing driver 98 p start driving the imagestabilizing mechanism 95 according to the determined shake correctiontarget value to perform the shake correction.

The corrections are performed for both the rotational shake and theshift shake for the first time hereat.

At step S1011, if the half-press operation S1 of the release member 93 ais changed to off, the flow proceeds to step S1012, and if thehalf-press operation S1 is continued, the flow returns to step S1006.

In other words, the shake correction is continued with the gain of theshake correction target value altered depending on the imagemagnification and/or the sensitivity that change depending on the imagepickup distance (or object distance), as long as the half-pressoperation S1 is continued, and it is assumed that, during the shakecorrection, there is no variation in the posture of the accelerometer 11p.

Incidentally, if the lens 90 is in-focus state, the focus lens 99 is notdriven for focusing, and if an in-focus state is not detected (forexample, the subject is moved), the focus lens 99 is driven for focusingat step S1007 and the image pickup distance is again detected to alterthe image pickup magnification at step S1008.

At step S1012, the drive of the image stabilizing mechanism 95 isstopped, and the flow returns to step S1001 to wait for the half-pressoperation S1 is performed again.

As described above, in Embodiment 1, only rotational shakes are firstcorrected, and then shift shakes are corrected.

Since the rotational shake has been corrected before focusing, thefocusing accuracy can be increased and accurate information needed forthe shift shake correction (i.e. image pickup magnification) can beobtained.

The details of the angular velocity integrator 13 p and the accelerationintegrator 22 p shown in FIG. 2 will now be described.

As described above, the angular velocity integrator 13 p typicallyintegrates a high frequency component of 0.1 Hz or higher to convert itto the shake angle signal, and the acceleration integrator 22 ptypically integrates a high frequency component of 0.4 Hz or higher toconvert it to the shake displacement signal.

FIGS. 6A and 6B show gain integration characteristics of theacceleration integrator 22 p and the angular velocity integrator 13 p,respectively; the horizontal axis 51 shows the frequency, and thevertical axis 52 shows the gain. The gain represents a ratio of themagnitude of an output signal to an input signal in terms of dB.

In FIG. 6A, a graph 53 shows the frequency characteristics in theacceleration integration in the normal state. The accelerationintegrator 22 p has a characteristic which performs a double integrationon a frequency component higher than 0.4 Hz (i.e. the accelerationsignal decreases in an inversely proportional manner to the square ofthe frequency), and attenuates a frequency component lower than 0.4 Hz(practically, a frequency component lower than 0.3 Hz: the accelerationsignal decreases as the frequency is lowered).

A graph 54 shows the frequency characteristics in the accelerationintegration upon activation of the accelerometer 11 p or when panning.Similarly to the graph 53, the acceleration integrator 22 p has acharacteristic which performs a double integration on a frequencycomponent higher than 0.4 Hz (i.e. the acceleration signal decreases inan inversely proportional manner to the square of the frequency).However, the acceleration integrator 22 p has a characteristic whichattenuates a frequency component below a frequency higher than that inthe normal state (1 Hz in this case: the acceleration signal decreasesas the frequency is lowered).

In FIG. 6B, a graph 55 shows the frequency characteristics in theangular velocity integration in the normal state. The angular velocityintegrator 13 p has a characteristic which performs single integrationon a frequency component higher than 0.1 Hz (i.e. the angular velocitysignal decreases in an inversely proportional manner to the frequency),and attenuates a frequency component lower than 0.1 Hz (i.e. the angularvelocity signal decreases as the frequency is lowered).

A graph 56 shows the frequency characteristics in the angular velocityintegration upon activation of the angular velocity meter 96 p or whenpanning. Similarly to the graph 55, the angular velocity integrator 13 phas a characteristic which integrates a frequency component higher than0.1 Hz (i.e. the angular velocity signals decreases in an inverselyproportional manner to the frequency). However, the angular velocityintegrator 13 p has a characteristic which attenuates a frequencycomponent below a frequency higher than that in the normal state (2 Hzin this case: the angular velocity signal decreases as the frequency islowered).

FIGS. 6C and 6D show phase characteristics of the accelerationintegrator 22 p and the angular velocity integrator 13 p, respectively;the horizontal axis 51 shows the frequency, and the vertical axis 57shows the phase. The phase represents a deviation angle of an outputsignal from an input signal.

In FIG. 6C, a graph 58 shows the phase/frequency characteristics in theacceleration integration in the normal state. For example, the phaseshift of an output relative to an input at 1 Hz is approximately −120degrees.

A graph 59 shows the phase/frequency characteristics upon activation ofthe accelerometer 11 p or when panning.

In FIG. 6D, a graph 510 shows the phase/frequency characteristics in theangular velocity integration in the normal state. For example, the phaseshift of an output relative to an input at 1 Hz is −78 degrees.

A graph 511 shows the phase/frequency characteristics in the angularvelocity integration upon activation of the angular velocity meter 96 por when panning.

In comparison with a computation using the integration result on acomponent of 0.1 Hz as shown in FIGS. 6B and 6D, a computation using theintegration result on a component of 0.4 Hz or higher as shown in FIGS.6A and 6C is represented as “having a narrow signal processing band.”

A phase shift and the shake correction accuracy will now be described.

An output (or displacement) obtained by performing a double integrationon an acceleration shown in FIG. 6C ideally lags 180 degrees in phase.

This can be explained by the fact that a single integration on a sinewave generates a cosine wave to change in phase by 90 degrees, and afurther single integration on the cosine wave generates a minus sine (ora phase of −180 degrees).

If such an ideal integration can be used to compute a displacement,shakes could be perfectly corrected.

However, the ideal integration is not preferable in camera manipulation.

One reason is that all errors of DC components are accumulated.

Therefore, a component of a frequency above a predetermined frequency(for example, 0.4 Hz) is integrated as seen from the frequencycharacteristics shown in FIG. 6C, and a component of a frequency lowerthan the predetermined frequency is attenuated.

However, if the integration and the low frequency attenuation are set inthis way, the shake correction accuracy in a hand shake frequency band(for example, from 1 Hz to 10 Hz) is reduced.

This is because, as shown in FIG. 6C, the phase shift at 1 Hz is not−180 degrees; the phase lags only up to −120 degrees.

Therefore, image shakes due to a hand shake of 1 Hz cannot besufficiently corrected.

Incidentally, in the case of a hand shake of 10 Hz, FIG. 6C shows −170degrees in phase, and the shake correction accuracy is maintained.

The above description has been made as to a problem when it is assumedthat the shift shake has the same characteristic as the rotationalshake, the problem having been a bottleneck in the shift shakecorrection so far.

However, detailed investigations on the shift shake have revealed thatthe shift shake has a different characteristic from that of therotational shake.

FIG. 7 shows the frequency characteristics of the shift shake; thehorizontal axis 51 shows the frequency, and the vertical axis 61 showsthe amount of an image shift on the image plane due to the shift shake.

A graph 62 shows the amount of an image shift due to the shift shake,and it has been found that attenuation is observed in both low and highfrequencies across 2 Hz.

This indicates that the frequency band is narrower in comparison withthe rotational shake (which has a frequency band from 1 Hz to 10 Hz).

Therefore, if the shift shake is corrected with the characteristicsshown in FIGS. 6A and 6C, the amount of the image shift on exposure willbe acceptable.

Incidentally, an output (or angle) obtained by performing a singleintegration on the angular velocity shown in FIG. 6D ideally lags 90degrees in phase.

This can be explained by the fact that a single integration on a sinewave generates a cosine wave to change in phase by 90 degrees.

In FIG. 6D, the phase shift at 1 Hz is −78 degrees, which is close to−90 degrees, so that the rotational shake can be sufficiently corrected.

Here, if the frequency band in which the characteristics shown in FIG.6D are provided is narrowed as with shift shake, the correction accuracyof the rotational shake is significantly degraded. This is because therotational shake includes a lower frequency shake than the shift shake.

Using a narrow integration band and a reduced ability of integration inlow frequencies as shown in computational characteristics of FIGS. 6Aand 6C reduces accumulation of errors superimposed on the accelerometer,so that an acceptable level of accuracy of the accelerometer can belowered, and therefore a small and lightweight accelerometer can beused.

Additionally, with a small time constant (a characteristic of theintegration performed from 0.4 Hz is represented as “having a small timeconstant” as compared with a characteristic of the integration performedfrom 0.1 Hz), activation of the computation can be accelerated.

As described above, the rotational shake correction is previouslyactivated, followed by activation of the shift shake correction after anin-focus state is obtained, which will have the benefit of acceleratedactivation from the small time constant.

Referring now to the characteristics shown in FIGS. 6A and 6B, thegraphs vary upon activation and panning as shown in the graphs 54 and56.

Therefore, the frequency characteristics of the two may possibly bematched upon activation and panning.

However, the frequency characteristics in the normal state are differentfrom each other as shown in the graphs 53 and 55 (the integration bandin FIG. 6A is narrower, or smaller in the time constant, than that inFIG. 6B).

The embodiment is characterized in that the computation band for therotational shake is different from that for the shift shake in thenormal state (excepting upon activation and panning).

Although description has been made as to the case where the computationprocessing bands are different between the angular velocity integrator13 p and the acceleration integrator 22 p shown in FIG. 2, the DCremoving circuit and the high-frequency attenuation circuit for removinga high-frequency noise component in the amplifiers 12 p and 20 p mayhave different computation processing bands. In addition, the combinedfrequency band of the angular velocity integrator 13 p with theamplifier 12 p may be different from the combined frequency band of theacceleration integrator 22 p with the amplifier 20 p.

As described above, the embodiment takes into account the fact that thefrequency band of the rotational shake is different from that of theshift shake, and has integration characteristics for the shift shakedifferent from integration characteristics for the rotational shake toreduce accumulation of errors generated in the double integration, sothat a small and lightweight accelerometer, which is usable to consumerproducts, can be used.

Embodiment 2

FIGS. 8A and 8B show characteristics of Embodiment 2 according to thepresent invention. FIG. 8A shows the frequency characteristics of thegain, and FIG. 8B shows the frequency characteristics of the phase.

In FIGS. 8A and 8B, the acceleration integrator 22 p is provided with afrequency compensator for causing the phase to lag with respect to thecharacteristics as shown in FIGS. 6A and 6C. The frequency compensatorcauses the phase of input signals of a low frequency to lag.Alternatively, it causes the phase of input signals of a lower frequencyto lag in comparison with the angular velocity integrator 13 p.

The frequency compensator for causing the phase of the input signals ofa low frequency to lag is composed of, for example, a low-pass filter,and attenuates signals having a frequency higher than 5 Hz, as indicatedby a long dashed double-short-dashed line as a graph 71.

Therefore, the shift shake of 5 Hz or higher cannot be accuratelycorrected. However, this will not pose a significant problem evenwithout the shake correction because practically little shift shake ispresent in the frequency band.

However, with the low-pass filter inserted, the phase shift at 2 Hz iscompensated close to −180 degrees as shown in a graph 72 in FIG. 8B (inthe graph 58, the phase shift at 2 Hz is −148 degrees).

This, therefore, provides for more accurate correction of the shiftshake.

The characteristics of the low-pass filter (i.e. 5 Hz or higher isattenuated) may also be variable depending on an image pickup conditionof the camera such as the state of a camera shake or the imagemagnification (for example, 10 Hz or higher is attenuated) so thatnecessary characteristics are obtained for a particular state.

As described above, the embodiment takes into account the fact that thefrequency band of the rotational shake is different from that of theshift shake, and has integration characteristics for the shift shakedifferent from integration characteristics for the rotational shake toreduce accumulation of errors generated in the double integration, sothat a small and lightweight accelerometer, which is usable to consumerproducts, can be used.

Embodiment 3

In Embodiments 1 and 2, the angular velocity integrator 13 p and theacceleration integrator 22 p in the lens CPU 97 perform computation (forexample, a digital filter using the bilinear transformation) to obtaindesired integration characteristics and DC cut off characteristics (i.e.attenuation of a low frequency). The computation band of the angularvelocity integrator 13 p and that of the acceleration integrator 22 pare different from each other. Alternatively, a phase compensationfilter is provided for the acceleration integrator 22 p.

A similar configuration may also be obtained by the amplifiers 12 p and20 p that are analog circuits, which are provided before the lens CPU97. The cooperative operation of the amplifiers 12 p and 22 p, which areanalog circuits, and the angular velocity integrator 13 p and theacceleration integrator 22 p, which perform digital computation, canprocess signals separately and optimally for the rotational shake andthe shift shake.

FIG. 9 shows an exemplary configuration of the amplifiers 12 p and 20 pin this case.

In FIG. 9, the amplifier 12 p for the angular velocity meter 96 p iscomposed of computation amplifiers 80 a and 81 a, multiple resistors,and capacitors.

A product of the resistor 83 a and the capacitor 84 a defines a DC cutoff ability (or a low frequency attenuation ability); in this case, forexample, the resistor 83 a having 1.5 MΩ and the capacitor 84 a having2.0 μF are used to attenuate angular velocity signals having a frequencyof 0.05 Hz or lower.

In addition, the computation amplifier 80 a has a combined function forthe signal as a buffer amplifier and an amplifier having anamplification factor of 40 times.

A product of the resistor 86 a and the capacitor 85 a defines ahigh-frequency noise cut off ability (or a high frequency attenuationability); in this case, for example, the resistor 86 a having 200 kΩ andthe capacitor 85 a having 2.7 nF are used to attenuate angular velocitysignals having a frequency of 300 Hz or lower.

A switch 82 a switches time constants for DC cut off. Upon activation orwhen a large panning occurs, the switch 82 a causes the capacitor 84 ato immediately charge in response to an instruction from the lens CPU 97so that signals are rapidly stabilized.

The output from the amplifier 12 p is input to the lens CPU 97, anddigitally integrated and subjected to the DC cut off in the angularvelocity integrator 13 p.

As shown in a block diagram of the angular velocity integrator 13 p ofFIG. 9, the digital integration has a characteristic of performing asingle integration on a frequency component higher than 0.1 Hz andattenuating a frequency component lower than 0.1 Hz.

Similarly, in FIG. 9, the amplifier 20 p of the accelerometer 11 p iscomposed of computation amplifiers 80 b and 81 b, multiple resistors,and capacitors.

A product of the resistor 83 b and the capacitor 84 b defines a DC cutoff ability (or a low frequency attenuation ability); in this case, forexample, the resistor 83 b having 400 kΩ and the capacitor 84 b having1.0 μF are used to attenuate acceleration signals having a frequency of0.4 Hz or lower.

In addition, the computation amplifier 80 b has a combined function forthe signal as a buffer amplifier and an amplifier having anamplification factor of 40 times.

A product of the resistor 86 b and the capacitor 85 b defines ahigh-frequency noise cut off ability (or a high frequency attenuationability) and is responsible for the phase compensation as described inEmbodiment 2. In this case, for example, the resistor 86 b having 200 kΩand the capacitor 85 b having 150 nF are used to attenuate accelerationsignals having a frequency of 5 Hz or lower.

A switch 82 b switches time constants for DC cut off. Upon activation orwhen a large panning occurs, the switch 82 b causes the capacitor 84 bto immediately charge in response to an instruction from the lens CPU 97so that signals are rapidly stabilized.

The output from the amplifier 20 p is input to the lens CPU 97, anddigitally integrated and subjected to the DC cut off in the accelerationintegrator 22 p through the acceleration gravity corrector 21 p.

As shown in a block diagram of the acceleration integrator 22 p of FIG.9, the digital integration has a characteristic of performing a doubleintegration on a frequency component higher than 0.4 Hz and attenuatinga frequency component lower than 0.4 Hz.

In this way, the amplifier 20 p is responsible for the phasecompensation, so that a phase shift due to the narrow integration bandof the shift shake is compensated.

In addition, the DC cut off frequency of the amplifier 20 p is at 0.4Hz; the attenuation starting on a higher frequency side than 0.05 Hz ofthe amplifier 12 p prevents errors in accelerometer outputs fromaccumulating.

Incidentally, although the example in FIG. 9 shows the case where theintegration bands of the angular velocity integrator 13 p and theacceleration integrator 22 p are different from each other (theacceleration integrator 22 p has a smaller integration band), differentprocessing frequency bands may be achieved only in the amplifiers 12 pand 20 p, with the same integration bands provided for the block.

According to the embodiments described above, a small and lightweightaccelerometer can be used to sufficiently correct the shift shake.

Additionally, although description has been made in each Embodimentabove as to an exemplary solution for addressing the shift shake tocorrect an image shake in a digital camera, the image stabilizingapparatus in the embodiments can be constructed in a small and highlystable mechanism, so that the present invention is not limited to thedigital camera and it can be applied to a digital video camera,monitoring camera, Web camera, mobile phone and the like.

Although description has been made in the embodiments as to the casewhere the correction lens 95 a is shifted relative to the optical axis91 to correct image shakes, the present invention may also be applied tothe case where the image pickup element 94 is shifted relative to theoptical axis 91 to correct image shakes.

Furthermore, the present invention is not limited to these preferredembodiments and various variations and modifications may be made withoutdeparting from the scope of the present invention.

This application claims foreign priority benefits based on JapanesePatent Application No. 2006-029966, filed on Feb. 7, 2006, which ishereby incorporated by reference herein in its entirety as if fully setforth herein.

1. An image stabilizing apparatus comprising: an angular velocitydetector which detects angular velocity acting on the image stabilizingapparatus; an angular velocity computing unit which processes an angularvelocity signal obtained by the angular velocity detector, the angularvelocity computing unit processing the angular velocity signal with afirst frequency characteristic; an acceleration detector which detectsacceleration acting on the image stabilizing apparatus; an accelerationcomputing unit which processes an acceleration signal obtained by theacceleration detector, the acceleration computing unit processing theacceleration signal with a second frequency characteristic having asignal processing band narrower than the first frequency characteristic;an adder which adds an output signal from the angular velocity computingunit to an output signal from the acceleration computing unit; and animage stabilizing mechanism which performs an image stabilizingoperation based on an output signal from the adder, wherein a gravityacceleration component of the output signal from the accelerationcomputing unit is corrected using the output signal from the angularvelocity computing unit.
 2. The image stabilizing apparatus according toclaim 1, wherein a cut off frequency processed by the accelerationcomputing unit is higher than a cut off frequency processed by theangular velocity computing unit.
 3. The image stabilizing apparatusaccording to claim 1, wherein the acceleration computing unit has afrequency compensation function for providing a phase lag to a lowfrequency input signal.
 4. An optical apparatus comprising the imagestabilizing apparatus according to claim 1.